Nonnegative Solutions for a Class of Nonpositone Problems
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1 Claremont Colleges Claremont All HMC Faculty Publications and Research HMC Faculty Scholarship Nonnegative Solutions for a Class of Nonpositone Problems Alfonso Castro Harvey Mudd College Ratnasingham Shivaji Mississippi State University Recommended Citation A. Castro and R. Shivaji. Non-negative solutions for a class of non-positone problems, Proc. Royal Soc. Edinburgh, 108A, (1988), pp This Article is brought to you for free and open access by the HMC Faculty Scholarship at Claremont. It has been accepted for inclusion in All HMC Faculty Publications and Research by an authorized administrator of Claremont. For more information, please contact scholarship@cuc.claremont.edu.
2 Proceedings of the Royal Society of Edinburgh, 108A, , 1988 Non-negative solutions for a class of non-positone problems Alfonso Castro Department of Mathematics, North Texas State University, Denton, TX , U.S.A. and R. Shivaji Department of Mathematics, Mississippi State University, Mississippi State, MS 39762, U.S.A. (MS received 12 February Revised MS received 11 September 1987) Synopsis In the recent past many results have been established on non-negative solutions to boundary value problems of the form -u"(x) = Xf{u(x)); 0<x<l, M(0) = 0 = K(1), where A>0, /(0)>0 (positone problems). In this paper we consider the impact on the non-negative solutions when /(0) < 0. We find that we need f(u) to be convex to guarantee uniqueness of positive solutions, and f(u) to be appropriately concave for multiple positive solutions. This is in contrast to the case of positone problems, where the roles of convexity and concavity were interchanged to obtain similar results. We further establish the existence of non-negative solutions with interior zeros, which did not exist in positone problems. 1. Introduction Consider the two point boundary value problem where A > 0 is a constant and / e C 2 satisfies -U"(X) = A/(W(JC)); *e(0,l), (1.1) «(0) = 0 = u(l), (1.2) 0. (1.3) Firstly, note that any solution u(x) of (1.1) (1.2) is symmetric about any point x o e(0, 1) such that u'(x o ) = 0. Then by (1.3) it is possible that a non-negative solution u(x) of (1.1) (1.2) may have interior zeros in (0,1). (This was not the case when/(0) >0, where if u(x) is a non-negative solution of (1.1) (1.2), then u{x) > 0 on (0,1).) We will distinguish those solutions which do not have interior zeros by referring to them as positive solutions. We shall consider three distinct cases: Case (A). f"(s)>0 for s >0, Case(B). f"(s)<0 for s >0,
3 292 Alfonso Castro and R. Shivaji Case (C). There exists some s 0 such that/%y) < 0 for 0<s<s o for s > s 0. Our main results are: and/"(y)>0 THEOREM 1.1. Letf(0) < 0, f'(s) >0fors>0 and p\ 6 be positive real numbers that satisfy /(/3) = 0, F(6) = 0, respectively, where F(s) = fof(t) dt. Case (A). If f"(s)>0 for s>0 and lim f(s)/s = +oc, then there exist A* >0 such that (1.1) (1.2) have a unique positive solution for 0< A^A* and have no positive solutions for A>A*. Also denoting by p k the supremum norm of the positive solution, p A increases as A decreases, and in particular, p A. = 6, limp A = +oo. (See Fig. 1.1.) A-»0 Case (B). // f"(s)<0 for s>0, lim f(s) = M where 0<A/^+oo, lim sf'(s) = 0 and (J(6)/d) <f'(6), then there exist A*, fi x such that 0 < /i, < A* and (1.1) (1.2) have no positive solutions for 0 < A < fi x and at least one positive solution for h = Hi. Further (1.1) (1.2) have at least two positive solutions for jui<a^ A* and there exists ^2 = A* such that (1.1) (1.2) have a unique positive solution for A > ju 2. Also, p A. = 6 and lim p A = +<*>. (See Fig. 1.2.) f(s) F{s) 0 A* Figure 1.1. Bifurcation diagram (Theorem 1.1, Case (A)).
4 Non-negative solutions for a class of non-positone problems 293 f(s) fi Figure 1.2. Bifurcation diagram (Theorem 1.1, Case (B)). Case (C). Iff"(s) <0forse (0, s 0 ) with s o > 6, f"(s) >0fors>s o, (f(d)/6) < f'{d), and if there exists o>d such that H(o) = F(o) - (o/2)f(o) > 0, lim (f(s)/s) = + and lim f(s) lim sf'(s) < 0, then there exist A*, A x, A 2 such f/iaf 0 < Aj < A* ^ A 2 and (1.1) (1.2) have a unique positive solution for 0 < A < Aj and no positive solutions for A > A 2. Further, there exists a range for A in (A x, A*) in which (1.1)-(1.2) have at least three positive solutions and if A 2 >A* then (1.1) (1.2) have at least two positive solutions for A e [A*, A 2 ). Also p A. = 6 and lim p x = +oo. (See Fig. 1.3.) A 0 LEMMA 1.2. Let a = 0 2 /[-F(/3)]. 77ien 2a- ^ A* ^ 8a-. LEMMA 1.3. If u x (x) and u 2 (x) are distinct positive solutions o/(l.l) (1.3), then {x e (0, l)/u!(x) = u 2 (x)} is the empty set. THEOREM 1.4. Let the hypotheses of Theorem 1.1 hold. Then in each of the cases (A), (B), or (C), given n a positive integer, (1.1) (1.2) have a non-negative solution with n interior zeros if and only if A = (n + 1) 2 A*. Further, such a solution is unique.
5 294 Alfonso Castro and R. Shivaji fis) Fis) 4- A, A* = A 2 A, A A 2 Figure 1.3. Bifurcation diagram (Theorem 1.1, Case (C)). I Remark 1.5. The above results on positive solutions are in contrast to the case of positone problems (see [l]-[3]) where concavity (not convexity) guaranteed uniqueness while convexity (not concavity) allowed multiplicity to be a possibility. Remark 1.6. Our results are related to the fact that the Hessian of the variational functional corresponding to -u"(x) =/(«(*))-/(0); 0<*<l is non-singular at a positive solution. However, our assumptions are quite general and as such are not enough to guarantee the above. Remark 1.7. Unlike the case of positone problems where /(0)>0, here, in general, it seems rather difficult to apply the method of sub-super solutions to track down the positive solutions. This is because /(0) < 0 makes xp = 0 a supersolution and not a subsolution as in the case of positone problems. In fact,
6 Non-negative solutions for a class of non-positone problems 295 for many of these solutions we suspect that it will not be possible to use this method. However, see [4], where boundary value problems of the type AM = A(M - u 3 ) - e; u = 0; xeqcr", xedq, were considered, and existence of positive solutions for a certain range of A and e > 0 small enough were derived, using sub-super solutions via the anti-maximum principle due to P. Clement and L. A. Peletier. Remark 1.8. See [5], where (1.1) (1.3) are considered when f"(u)<0 and when / satisfies certain additional hypotheses which are not easy to verify in general. The authors prove that, at most, there are only two positive solutions for any A. We shall prove our results in Section 2. In Section 3 we give an example satisfying the hypotheses of Theorem 1.1. In particular, we discuss Case (C), as construction of examples for Cases (A) and (B) is much easier. 2. Proofs of results Proof of Theorem 1.1. On multiplying (1.1) by u'(x) and integrating, we obtain Since we are dealing with positive solutions, u{x) has to be symmetric with respect to x = 1/2 and u'{x) > 0 for x e (0, \), see Figure 2.1 In fact, if p = Sup u{x) then u{\) = p, p = 6, and substituting x = \ in (2.1) we obtain * e((u) Now integrating (2.2) on [0,x] and using (1.2), we obtain du rvf(p)-f(«)' (2.2) (2.3) u(x) 1/2 Figure 2.1
7 296 Alfonso Castro and R. Shivaji His) Figure 2.2 and hence substituting x = \ in (2.3) we have du :=G(p). (2.4) Now for positive solutions p must be in [d, c). In fact, for given A such that there exists a p e [8, ) for which G(p) = VX, it follows that (1.1) (1.2) have a positive solution u(x) given by (2.3) such that Sup u(x) = u{\) = p. Further, it follows xe(0,l) that G(p) is a continuous function and differentiable for p e (6, o) with where = F(s)-(s/2)f(s). (2.5) (2.6) Case (A). We will prove that G'(p)<0 and lim G(p) = 0. Now H'(s) = 2[f(s)-sf'(s)] and H"(s) = -($)sf"(s). But /(0)<0, f"(s)>0 for s >0. Thus H'(s) < 0 for s > 0, see Figure 2.2. Hence H(p)-H(pv)<0 note that for p e (6, <»), for v e [0, 1], and consequently G'(p)<0. Next, G(p) = (2.7) Let L(u): = F(pu)/F(p). Then L(0) = 0, L'(v) = (f(pv)p)/f(p) and L» = (f'{pv)p 2 )/F(p). But /(s) < 0 for 5 e (0, /5), /(s) > 0 for s > /S and /'(s) > 0 for s>0. Hence for a given p e (0, <»), L(U) takes the shape shown in Figure 2.3. Hence, clearly, L(v) ^ v for v e [0, 1]. Consequently from (2.7)
8 Non-negative solutions for a class of non-positone problems 297 L(v) dip Figure 2.3 But since lim f(s)/s = +, we have hence lim G(p) = 0. This completes the proof of Case (A). lim p 2 /F(p) = lim 2p//(p) = 0, and Case (B). Note that /(0) < 0, /"(s) < 0 for s > 0, /(0) < df'{6) and lim /( 5 ) = S» + 2C M. Thus H"(s) > 0 for s > 0, if'(s) < 0 for 5 e [0, 0] and lim if'(j) = (M/2) > 0. Hence there exists 6, y such that 0 < 5 < y, tf'(<5) = 0 and H(y) = 0, see Figure 2.4. Consequently, G'(p)<0 for p e [0, d] and G'(p)>0 for p ^ y and, in order to complete this part of the proof it remains to prove that lim G(p) = +. Now L{v) = F(pv)lF{p) ^ [f(0)pv]/f(p), since F" =/' > 0. Hence from (2.7) H(s) Figure 2.4
9 298 we have Alfonso Castro and R. Shivaji dv - [(f(o)pv)/f(p)] -(/(O)p)AF(p) = -V2(VF(p)//(0))[ where w = (f(0)pv)/f(p). Hence G(p)s-2V5(VF(P)//(O)){[1- But lim p/f(p) = while lim p 2 /F(p) = lim 2p//(p) = +=c. Hence lim G(p) = + and Case (B) is proved. Case (C). The hypotheses imply that H(s) takes the form shown in Figure 2.5, which shows a 1, a 2, o 3 and CT 4. Hence H(p) H(pv)<0 for u e [0, 1) when p e [6,CTJand when p>o 4, while //(p) - H(pv) > 0 for v 6 [0, 1) when p e (cr 2. ^l- Consequently G'(p) < 0 for p e [6, o x ] and for p a 4, while G'{p) > 0 for p 6 [CT 2, ^3]- Now to complete the proof of Theorem 1.1 it remains to prove that lim G{p) = 0, which follows by arguments identical to those used in the proof of Case (A). Proof of Lemma 1.2. First we note that (1 - V-F(s)) g (l/v--f(/3)) for His) Figure 2.5
10 Non-negative solutions for a class of non-positone problems 299 F(s) Figure 2.6 s e (0, 6), and since F"(s) =f'(s) > 0 for s > 0 we have (See Fig. 2.6.) Thus Hence K) \-[F(P)/(d-P)](6-s) for. fvj8/(-f(j8)s) for 0^5^/3, ^ for (2.8) and {-F{p)) 2Vjs = 2y/26N-F(fi). (2.9) From (2.8) and (2.9) it easily follows that 2cr^ A* = [G(0)] 2^8a, where o- = 6 2 /[ F(P)], and Lemma 1.2 is proved. Note here that for A = A* the minimal solution u(x) has supremum norm p = 8 and hence u'(0) = 0, see Figure 2.7.
11 300 Alfonso Castro and R. Shivaji - V- 2(n + Figure 2.8 Proof of Lemma 1.3. If «2 (2) = Pi> "1(2) = Pi, then at any point * o 6 (0, \) where Ui(x 0 ) = u 2 (x 0 ), from (2.2) we must have w 2 (*o) > "i(*o)- Hence, there can be at most one such point. But from (2.2) we also have u 2 (0) > uj(o). Thus, no such point exists. Proof of Theorem 1.4. First we note that in order to study a non-negative solution with n interior zeros, due to the symmetry we need to study the solution only in the interval [0, l/(2(n + 1))], see Figure 2.8. From (2.1) we have for x e [0, l/(2(/i + 1))], «'(*) = V2A[F(p)-F(u)], (2.10) where p = sup u(x) = u(l/(2(n +1))). But since we must have u'(0) = 0, F(p) = 0 and hence p = 6. Now integrating (2.10) on [0, x], we obtain ru(x) JO ^ du xe[0,l/(2(n and hence substituting x = l/(2(n + 1)) in (2.11) we must have du (2.11) (2.12) Thus, in order to have a non-negative solution u(x) to (1.1) (1.2) with n interior zeros, A must equal (n + 1) 2 A* and Sup u(x) = 6. In fact, given A = (n + 1) 2 A* it follows that (1.1) (1.2) have a unique non-negative solution u{x) with n interior zeros given by (2.11) with Sup u{x) = «(l/(2(n + 1))) = An example This example illustrates Theorem 1.1, Case (C). Consider f(s) = s 3 - as 2 + bs-c, (3.1)
12 Non-negative solutions for a class of non-positone problems 301 where a > 0, b>0, c > 0 and they satisfy Clearly /(0) < 0. Further ft>(32/81)a 2, (3.2) fl 3 >54c. (3.3) f'(s) = 3s 2-2as + b = 3{[s-(a/3)] 2 + (b/3)-(a 2 /9)}. (3.4) But (3.2) implies that (ft/3) > {a 2 19). Hence /'(*)>0 for s>0 and since lim f(s) = +, there exists a unique /? > 0 such that /(/3) = 0. Next F(s) = sg(s), where and g(s) = (s 3 /4) - (as 2 /3) + (bs/2) - c, (3.5) g'(s) = (3s 2 /4) - (2os/3) + (ft/2) = (3/4){[s - (4a/9)] 2 + (2ft/3) - (16a 2 /81)}. (3.6) Once again (3.2) implies that (2ft/3)> (16a 2 /81) and hence g'(.s)>0 for s 0. But g(0) < 0 and lim g(s) = +oo. Hence there exists a unique 6 > j3 such that Now note that f"(s) = 6s-2a. (3.7) Clearly there exists s 0 = (a/3) such that f"(s) < 0 for s e (0, s 0 ) and f"(s) > 0 for s>s 0. Also (3.2), (3.3) imply that Hence 6<s o = (a/3). Next consider F(a/3) = (a/3){(a 3 /108) - (a 3 /27) + (aft/6) - c} = (a/3){(ab/6)-c-(a 3 /36)} i= (a/3){(32fl 3 /486) - (a 3 /54) - (a 3 /36)} = (19a 4 /2916)>0. (3.8) f(6) - df'(d) = -2d 3 + a6 2 - c. Now g(6) = 0 and thus substituting for c we have f(6) - 6f'(6) = (-90 3 /4) + (4a0 2 /3) - (bd/2) = (~96/4){[d - (8a/27)] 2 + (6ft/27) - [64«2 /(27) 2 ]}. Hence, using (3.2), we have f(9)-df'(8)< 0. Finally, the hypotheses lim (f(s)/s) = + and lim f(s) - lim sf'(s)<0 are easily seen to be satisfied, and hence it remains to prove the existence of a
13 302 Alfonso Castro and R. Shivaji number a > 0 such that H(o) > 0. Inequality (3.3) implies that //(a/3) = (-a 4 /324) + (a 4 /162) - (ac/6) = {[a 4-54ac]/324} >0, and (a/3) > 6. Hence the result. References 1 K. J. Brown, M. M. A. Ibrahim and R. Shivaji. 5-shaped bifurcation curves. Nonlinear Anal. 5 (1981), R. Shivaji. Uniqueness results for a class of positone problems. Nonlinear Anal. 2 (1983), T. W. Laetsch. The number of solutions of a nonlinear two point boundary value problem. Indiana Univ. Math. J. 20 (1970/71), K. J. Brown and R. Shivaji. Simple proofs of some results in perturbed bifurcation theory. Proc. Roy. Soc. Edinburgh Sect. A 93 (1982), P. Brunovsky and S. N. Chow. Generic properties of stationary state solutions of reactiondiffusion equations. /. Differential Equations 53 (1984), {Issued 27 April 1988)
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